Tunable Synthesis of Prussian Blue in Exponentially Growing

Aug 13, 2009 - Pierre Schaaf,*,‡ and Vincent Ball*,z,§. ‡Centre National de la Recherche Scientifique, Unit´e Propre de Recherche 22, Institut C...
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Tunable Synthesis of Prussian Blue in Exponentially Growing Polyelectrolyte Multilayer Films† )

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Nicolas Laugel,‡ Fouzia Boulmedais,‡ Alae E. El Haitami,z,§ Pierre Rabu, Guillaume Rogez, Jean-Claude Voegel,z,§ Pierre Schaaf,*,‡ and Vincent Ball*,z,§

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‡ Centre National de la Recherche Scientifique, Unit e Propre de Recherche 22, Institut Charles Sadron, 23 rue du Loess, BP 84047, 67034 Strasbourg Cedex 2, France, zInstitut National de la Sant e et de la Recherche M edicale, Unit e 977, 11 rue Humann, 67085 Strasbourg Cedex, France, §Universit e de Strasbourg, Facult e de Chirurgie Dentaire, 1 Place de l’H^ opital, 67000 Strasbourg, France, and Centre National de la Recherche Scientifique Universit e de Strasbourg, Unit e Mixte de Recherche 7504, Institut de Physique et Chimie des Mat eriaux de Strasbourg, 23 rue du Loess, BP 43, 67034 Strasbourg Cedex 2, France

Received April 26, 2009. Revised Manuscript Received July 12, 2009 Polyelectrolyte multilayer (PEM) films have become very popular for surface functionalization and the design of functional architectures such as hollow polyelectrolyte capsules. It is known that properties such as permeability to small ionic solutes are strongly dependent on the buildup regime of the PEM films. This permeability can be modified by tuning the ionization degree of the polycations or polyanions, provided the film is made from weak polyelectrolytes. In most previous investigations, this was achieved by playing on the solution pH either during the film buildup or by a postbuildup pH modification. Herein we investigate the functionalization of poly(allylamine hydrochloride)/poly(glutamic acid) (PAH/PGA) multilayers by ferrocyanide and Prussian Blue (PB). We demonstrate that dynamic exchange processes between the film and polyelectrolyte solutions containing one of the component polyelectrolyte allow one to modify its Donnan potential and, as a consequence, the amount of ferrocyanide anions able to be retained in the PAH/PGA film. This ability of the film to be a tunable reservoir of ferrocyanide anions is then used to produce a composite film containing PB particles obtained by a single precipitation reaction with a solution containing Fe3þ cations in contact with the film. The presence of PB in the PEM films then provides magnetic as well as electrochemical properties to the whole architecture.

Introduction The deposition of polyelectrolyte multilayer (PEM) films became a versatile and simple method to functionalize the surface of a broad range of materials in an easy and reproducible manner, allowing one to control the thickness of the film by playing on parameters such as the number of adsorption steps or the physicochemical parameters of the solution during the build-up of the film.1-5 The deposition of these coatings relies on the overcompensation of the surface charge of the substrate upon the deposition of a polyelectrolyte, hence allowing the deposition of an oppositely charged one.6-8 The successive deposition of two oppositely charged polyelectrolytes, separated by a rinsing step with a polyelectrolyte free solution, leads to a “layer pair”. The electrostatic interactions can be of very peculiar nature.9 Indeed, it has been found that the complexation enthalpy between the † Part of the “Langmuir 25th Year: Self-assembled polyelectrolyte multilayers: structure and function” special issue. *Corresponding author. Phone: þ33 (0)3 90 24 32 58; fax: þ33 (0)3 90 24 33 79; e-mail: [email protected] (V.B.). Phone: þ33 (0)3 88 41 40 12; e-mail: [email protected] (P.S.).

(1) Decher, G. Science 1997, 277, 1232. (2) Bertrand, P.; Jonas, A.; Laschewsky, A.; Legras, R. Macromol. Rapid Commun. 2000, 21, 319. (3) Hammond, P. T. Curr. Opin. Colloid Interface Sci. 1999, 4, 430. (4) Sch€onhoff, M. Curr. Opin. Colloid Interface Sci. 2003, 8, 86. (5) Ariga, K.; Hill, J. P.; Ji, Q. Phys. Chem. Chem. Phys. 2007, 9, 2319. (6) Caruso, F.; Donath, E.; M€ohwald, H. J. Phys. Chem. B. 1998, 102, 2011. (7) Ladam, G.; Schaad, P.; Voegel, J.-C.; Schaaf, P.; Decher, G.; Cuisinier, F. J. G. Langmuir 2000, 16, 1249. (8) Buron, C. C.; Fili^atre, C.; Membrey, F.; Perrot, H.; Foissy, A. J. Colloid Interface Sci. 2006, 296, 409. (9) Laugel, N.; Betscha, C.; Winterhalter, M.; Voegel, J.-C.; Schaaf, P.; Ball, V. J. Phys. Chem. B 2006, 110, 19443.

14030 DOI: 10.1021/la901479z

polycation and the polyanion used to build up the PEM films is endothermic when the buildup regime of the film is supralinear. This means that the interactions between the participating polyelectrolytes are driven by an entropy increase.9 In has also been demonstrated that the interactions allowing the buildup of such films are not only of pure electrostatic nature.10 The global entropy increase accompanying polyelectrolyte complexation is most probably due to counterion release, as it has been demonstrated for polycation-DNA complexation processes taking place in solution.11 The absence of small ions originating from the electrolyte solution in PEM films made from poly(diallyldimethyl ammonium chloride) (PDADMAC) and poly(4-styrene sulfonate) (PSS) first suggested the intrinsic charge compensation model in which the charge of the polyanions is exactly matched by the charge of the polycations in the bulk of the film.12 In the framework of this model, only the substrate-PEM film and PEM film-solution interfaces are charged. However, the charge compensation could also be of extrinsic nature, meaning that the ions from the electrolyte solution would contribute to the charge compensation of the PEM film. In this latter case, the PEM films should display a Donnan potential.13 Cyclic voltammetry (CV) experiments performed on PEM films made from different combinations of polyanions and polycations have shown that such films can be either impermeable or permeable to multivalent redox probes. Linearly growing PEM (10) (11) 3142. (12) (13)

Kotov, N. A. Nanostruct. Mater. 1999, 12, 789. Mascotti, D. P.; Lohman, T. M. Proc. Natl. Acad. Sci. U.S.A. 1990, 87, Schlenoff, J. B.; Ly, H.; Li, M. J. Am. Chem. Soc. 1998, 120, 7626. Calvo, E. J.; Wolosiuk, A. J. Am. Chem. Soc. 2002, 124, 8490.

Published on Web 08/13/2009

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films made from PSS and polycations seem to be totally impermeable to ferrocyanide (FCIV) when the number of deposited layer pairs is higher than about five.14-16 When the number of layer pairs is smaller, the film permeability to the redox probe strongly depends on the sign of the last deposited polyelectrolyte. Namely, when the topmost polyelectrolyte is of the same sign as the redox probe, it constitutes a barrier to the diffusion of the redox probe in the PEM film. However, the permeability of the linearly growing films can be modulated by the change in the nature of the electrolyte, the ionic strength, as well as the pH value used during or after its buildup.17 In general, an electrolyte of higher valence is more efficient for the doping process of PEM films with a multivalent redox probe.18 In the case of exponentially growing PEM films,19,20 whose structure is more hydrated, redox probes are able to diffuse and then are detectable electrochemically whatever the film thickness. In addition, charged redox probes can remain confined in the bulk of the film after the rinsing step with a solution free of the redox probe.21-23 As an interesting application of this observation, a reversible swelling/deswelling effect was observed for FCIV-containing poly(allylamine hydrochloride)/ poly(L-glutamic acid) (PAH/PGA) films during the FCIV oxidation/reduction cycle. These experiments have demonstrated the potential use of PEM films filled with redox species as electrochemical actuators, which could compete with films made from electroactive polymers.24 This ion incorporation can occur whatever the sign of the last deposited layer, with only around 20% differences in oxidation-reduction currents between positively and negatively charged ending layers.21 However, the films can be very selective with respect to the sign of the redox probe. The Donnan potential, positive or negative, displayed by the films is determined by the charge of the polyelectrolyte in excess inside the films, allowing the diffusion and preferential confinement of oppositely charged redox probes. The permeability and loading capacity of (PAH/PGA)n films with respect to ferricyanide were studied by Anzai and co-workers, who modified the pH during the film buildup to change the ionization degree of the weak polyelectrolytes.22,23 Another strategy was used by Zhang et al., who created selective permeability sites for ions.25 After the layerby-layer deposition of complexes made from polyelectrolytes and small ions and an oppositely charged polyelectrolyte, the small ions were released upon buffer rinsing, creating “ion traps” for ions of the same charge as those of the ions initially complexed. In the present investigation, we first aim at demonstrating that it is possible to modify the loading capacity in FCIV ions of an exponentially growing (PAH/PGA)n film without changing the pH of the external solution. The loading capacity was simply modified by a post-treatment of the film. Namely, after its buildup, the film was put into contact with either PGA- or PAH-containing solutions for variable times without any pH change. This was done because we suspected that the film is not in its equilibrium (14) Han, S.; Lindholm-Sethson, B. Electrochim. Acta 1999, 45, 845. (15) Farhat, T. R.; Schlenoff, J. B. Langmuir 2001, 17, 1184. (16) Pardo-Tissar, V.; Katz, E.; Lioubashevski, O.; Willner, I. Langmuir 2001, 17, 1110. (17) El Haitami, A. E.; Martel, D.; Ball, V.; Nguyen, H. C.; Gonthier, E.; Labbe, P.; Voegel, J.-C.; Schaaf, P.; Senger, B.; Boulmedais, F. Langmuir 2009, 25, 2282. (18) Salloum, D. S.; Schlenoff, J. B. Electrochem. Solid State Lett. 2004, E45. (19) Elbert, D. L.; Herbert, C. B.; Hubbell, J. A. Langmuir 1999, 15, 5355. (20) Picart, C.; Lavalle, Ph.; Hubert, P.; Cuisinier, F. J. G.; Decher, G.; Schaaf, P.; Voegel, J.-C. Langmuir 2001, 17, 7414. (21) H€ubsch, E.; Fleith, G.; Fatisson, J.; Labbe, P.; Voegel, J.-C.; Schaaf, P.; Ball, V. Langmuir 2005, 21, 3664. (22) Noguchi, T.; Anzai, J.-I. Langmuir 2006, 22, 2870. (23) Wang, B.; Anzai, J.-I. Langmuir 2007, 23, 7378. (24) Grieshaber, D.; V€or€os, J.; Zambelli, T.; Ball, V.; Schaaf, P.; Voegel, J.-C.; Boulmedais, F. Langmuir 2008, 24, 13668. (25) Chen, H.; Zeng, G.; Wang, Z.; Zhang, X. Macromolecules 2007, 40, 653.

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state, even if the deposition kinetics of either PAH or PGA was achieved after a few minutes.21,24 We hence make the assumption that the number of ion pairs between PGA and PAH may change after a post-treatment of the PEM film with one of its constituting polyelectrolytes. Moreover, the redox probe confinement in (PAH/PGA)n films has been used to induce the precipitation of an inorganic compound inside the film. Prussian Blue (PB) particles were obtained by diffusion of iron III ions into FCIVcontaining (PAH/PGA)n films. The post-treatment of a (PAH/ PGA)n film allows one to tune the FCIV concentration confined and then the amount of PB synthesized into the film. Therefore, the ion confinement in the PEM films allows one to prepare functional composite inorganic-organic hybrid materials, as it has been demonstrated using other strategies.26 Indeed, the powder obtained from the composite inorganic-organic hybrid film, with 20 cm2 area and a thickness of about 1 μm, has a measurable magnetic moment and displays a ferromagneticparamagnetic phase transition at low temperature, as expected for PB.

Experimental Section Solutions. All solutions were prepared with Milli-Q ultrapure water (F =18.2 MΩ 3 cm) from a Millipore system. Sodium nitrate (NaNO3), tris(hydroxymethyl aminomethane) base (Tris), nitric acid (HNO3), sulfuric acid, potassium ferrocyanide (K4Fe(CN)6, 3 H2O), iron(III) nitrate (Fe(NO3)3, 9 H2O), PGA (Mw = 4.4  104 g 3 mol-1), PAH (Mw =7.0104 g 3 mol-1) and poly(ethylene imine) (PEI) (Mw = 7.5  105 g 3 mol-1) were purchased from Aldrich and used without further purification. The buffer solution used in this work, unless otherwise specified, was 0.15 M NaNO3/ 0.01 M Tris with pH adjusted to 7.4 (( 0.1) by the addition of diluted HNO3 solution. We used nitrate salts instead of the traditional chloride salts because of the well-known adsorption of chloride ions on the surface of the gold working electrodes used in the CV experiments. Cyclic Voltammetry. A model CHI 604B potentiostat fitted with a Faraday cage (CH Instruments, Austin, TX) was used with a regular three-electrode setup. A double junction Ag/AgCl/KCl (3 M) electrode was used as a reference electrode (model CHI 111), a platinum wire was used as the counter electrode (model CHI 115), and a gold disk of 2 mm diameter was used as the working electrode. The gold working electrodes were treated before each experiment by two polishing cycles using aluminum oxide particles suspensions of 0.3 and 0.05 μm in diameter (Micropolish powder, Buehler), respectively. Each polishing cycle consisted in three polishing steps (2 min) with consecutive distilled water rinses. Each cycle ended with two ultrasound sonication steps, each one lasting over 3 min. Finally, the working electrodes were rinsed intensively with distilled water. The working electrodes were then activated through an electrochemical treatment consisting in 1000 CV sweep cycles between potential values of 0.2 and 1.6 V (vs Ag/AgCl), at a scan rate of 10 Vs-1 in a 0.5 M sulfuric acid solution. This activation step allows one to reproduce the surface chemistry of the gold/aqueous solution interface and to measure the surface roughness.27 The knowledge of the surface roughness is of prime importance for the calculation of the surface coverage in electroactive species because the real area accessible to the ions is higher than the geometric area of the electrode. Only activated electrodes having a roughness factor ranging from 2.2 to 3.5 were used for the subsequent CV and PEM film deposition experiments. A self-assembled monolayer of mercaptopropane sulfonate (MPS) was finally formed on the electrode to ensure a large surface charge before deposition of the PEM film. This was achieved by immersing the electrode in an aqueous solution (26) Chia, K.-K.; Cohen, R. E.; Rubner, M. F. Chem. Mater. 2008, 20, 6756. (27) Oesch, U.; Janata, J. Electrochim. Acta 1983, 28, 1237.

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containing 20 mM MPS and 16 mM sulfuric acid for 30 min, followed by a rinsing step of 5 min in a 16 mM sulfuric acid solution, following the protocol proposed by Mokrani et al.28 The electrode was finally dipped in the buffer solution before use in the electrochemical cell and/or adsorption of the multilayer film for at least 10 min. The electrode polishing, conditioning, and deposition of the MPS layer were performed before each new PEM deposition. Deposition of the PEM Films. The PEM films loaded with PB were obtained through three successive steps: (i) the buildup of the (PAH/PGA)n film, (ii) the confinement of FCIV ions in these films, and (iii) the synthesis of PB particles. The electrochemical characterization of the films was performed after each of these steps. (PAH/PGA)n films were obtained on the desired substrate by the layer-by-layer method using a computer-controlled dipping machine (Riegler & Kirstein, Berlin, Germany). The adsorbing scheme consisted of a 5 min dip in a given polyelectrolyte solution (either PAH or PGA) followed by rinsing in three dedicated beakers containing buffer solution: 205 s in the first one, 5  20 s in the second one, and 2  60 s in the third one. Repeating these deposition steps by alternating polycations and polyanions as the adsorbing species leads to the formation of a PEM film made from n layer pairs, (PAH/PGA)n. The major aim of this investigation was to study the influence of the last deposition step, regarding its polyanionic or polycationic nature as well as its dipping time. Namely, four post-treatments of the PEM films have been explored: the (PAH/PGA)10 film being dipped for 5 min or 8 h either in the PAH solution or in the PGA solution (with an intermediate PAH layer to ensure reversal of the surface charge at each deposition step in these latter cases). These films are thus noted, respectively, (PAH/PGA)10-PAH5min, (PAH/ PGA)10-PAH8h, (PAH/PGA)10-PAH/PGA5min, and (PAH/ PGA)10-PAH/PGA8h. PB Synthesis. Fe(CN)64- (FCIV) ions were confined in the polymeric film by a 5 h dip in a buffer solution containing 1 mM of FCIV ions, after which the confined quantity does not evolve anymore as measured by CV. The sample was then rinsed in three beakers containing the buffer solution, following the same pattern of rinsing times as the one described above for the deposition of the PEM film. The sample was finally let at rest in buffer solution for at least 1 h to allow the weakly bound FCIV ions to diffuse out of the coating before continuation of the experiment. PB particles were finally formed by dipping the PEM film with its confined FCIV anions in a buffer solution containing 1 mM iron(III) nitrate. The reaction that is expected to occur is described by eq 1: 3FeðCNÞ64 - þ4Fe3þ TFe4 ½FeðCNÞ6 3

ð1Þ 29,30

The precipitation reaction was allowed for at least 30 min. The sample was then rinsed in a manner identical to the one described in the previous paragraph. Ultraviolet-Visible (UV-Vis) Spectroscopy. All measurements were performed with an UV mc2 spectrophotometer (SAFAS, Monaco) used in the single beam mode. Quartz wafers (Thuet, Blodesheim, France) were used as substrates. Each wafer was cleaned by successive dipping for 30 min in a fuming hydrochloric acid/methanol (50:50 v/v) mixture and a 95% sulfuric acid solution. Each of these cleaning steps was followed by a rinsing step in distilled water. A first measurement was taken at this moment to ensure that no UV-vis absorbing material was present on the surfaces. The PEM film was then deposited following the protocol used for the gold electrodes, but without an MPS starting layer. The spectrum was acquired between 200 and 900 nm with a resolution of 1 nm after deposition of the PEM film, after immersion in the FCIV, and after immersion in the (28) Mokrani, C.; Fatisson, J.; Guerente, L.; Labbe, P. Langmuir 2005, 21, 4400. (29) Tyrasch, M.; Toutianoush, A.; Jin, W.; Schnepf, J.; Tieke, B. Chem. Mater. 2003, 15, 245. (30) Wang, Q.; Zhang, L.; Qiu, L.; Sun, J.; Shen, J. Langmuir 2007, 23, 6084.

14032 DOI: 10.1021/la901479z

Figure 1. Voltammograms of a gold working electrode coated with an MPS-(PAH/PGA)10 film in contact with a 1 mM FCIV solution (in 10 mM Tris, 150 mM NaNO3, pH 7.4 solution) for different times: (curve 1) a few seconds, (curve 2) 5 min, (curve 3) 30 min, and (curve 4) 60 min. The potential scan rate was 100 mV 3 s-1 in all cases. Fe(NO3)3-containing buffer. The reference transmission used to calculate the absorbance was that of the cleaned quartz slide.

Fourier Transform Infrared Spectroscopy in the Attenuated Total Reflection Mode (ATR-FTIR Spectroscopy). The PEMs were deposited according to the same protocol as for the UV-vis and CV experiments, but with the deposition of PEI as a starting layer, instead of MPS. This layer is mandatory to ensure good adhesion of the PEM film on the ZnSe crystal substrate. The PEM films were built in situ in the ATR cell (Graseby-Specac, Orpington, U.K.), and the spectrum of each layer was measured (Equinox 55 spectrometer, Bruker, Wissembourg, France) at a resolution of 2 cm-1 by accumulating 512 interferograms. The polyelectrolytes were dissolved in Tris-NaCl buffer made from D2O as in our previous studies.24 The absorbance was calculated as -log(Tlayer/TPEI), where Tlayer and TPEI represent the transmission in the presence of the considered film and when PEI is adsorbed on the naked ZnSe crystal. In the case of FCIV incorporation in the film, the reference spectrum for the absorbance calculation was that of the last deposited layer, either PGA5min, PGA8h, PAH5min, or PAH8h. The area under the peaks was calculated using the Origin 3.0 software.

Measurement of the Magnetic Properties of the PB Filled Films. The magnetic properties of the films were investigated by using an MPMS-XL Quantum Design SQUID magnetometer in the -5 to þ5 T and 1.8-300 K ranges. A few milligrams of powder samples (